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Technology, and Innovations"},{"name":"Advanced Technology Center"}],"content-domain":{"domain":["journals.aps.org"],"crossmark-restriction":true},"short-container-title":["Phys. Rev. Lett."],"accepted":{"date-parts":[[2026,8,17]]},"abstract":"<jats:p>\n                    We present a search of data from the first part of the fourth observing run of LIGO-Virgo-KAGRA for three kinds of dark matter\u2014dilatons (spin-0), dark photons (spin-1), and tensor bosons (spin-2)\u2014using three independent methods, each extended to search for all three candidates. Each dark matter candidate could interact with different standard-model particles in the instruments, causing unique differential strains on the interferometers. While we do not find any evidence for a signal, we place the most stringent upper limits to date on the couplings of each dark matter model to the interferometers. For scalars with masses between\n                    <a:math xmlns:a=\"http:\/\/www.w3.org\/1998\/Math\/MathML\" display=\"inline\">\n                      <a:mo stretchy=\"false\">[<\/a:mo>\n                      <a:mn>4<\/a:mn>\n                      <a:mo>\u00d7<\/a:mo>\n                      <a:msup>\n                        <a:mn>10<\/a:mn>\n                        <a:mrow>\n                          <a:mo>\u2212<\/a:mo>\n                          <a:mn>14<\/a:mn>\n                        <\/a:mrow>\n                      <\/a:msup>\n                      <a:mo>,<\/a:mo>\n                      <a:mn>1.5<\/a:mn>\n                      <a:mo>\u00d7<\/a:mo>\n                      <a:msup>\n                        <a:mn>10<\/a:mn>\n                        <a:mrow>\n                          <a:mo>\u2212<\/a:mo>\n                          <a:mn>13<\/a:mn>\n                        <\/a:mrow>\n                      <\/a:msup>\n                      <a:mo stretchy=\"false\">]<\/a:mo>\n                      <a:mtext>\u2009<\/a:mtext>\n                      <a:mtext>\u2009<\/a:mtext>\n                      <a:mi>eV<\/a:mi>\n                    <\/a:math>\n                    that couple to photons or electrons, our constraints on the scalar-to-electron or photon coupling improve upon those from the third observing run by 1 order of magnitude, with the tightest limit of\n                    <e:math xmlns:e=\"http:\/\/www.w3.org\/1998\/Math\/MathML\" display=\"inline\">\n                      <e:mrow>\n                        <e:mo>\u223c<\/e:mo>\n                        <e:msup>\n                          <e:mrow>\n                            <e:mn>10<\/e:mn>\n                          <\/e:mrow>\n                          <e:mrow>\n                            <e:mo>\u2212<\/e:mo>\n                            <e:mn>20<\/e:mn>\n                          <\/e:mrow>\n                        <\/e:msup>\n                        <e:mtext>\u2009<\/e:mtext>\n                        <e:mtext>\u2009<\/e:mtext>\n                        <e:msup>\n                          <e:mrow>\n                            <e:mi>GeV<\/e:mi>\n                          <\/e:mrow>\n                          <e:mrow>\n                            <e:mo>\u2212<\/e:mo>\n                            <e:mn>1<\/e:mn>\n                          <\/e:mrow>\n                        <\/e:msup>\n                      <\/e:mrow>\n                    <\/e:math>\n                    at a mass of\n                    <g:math xmlns:g=\"http:\/\/www.w3.org\/1998\/Math\/MathML\" display=\"inline\">\n                      <g:mo>\u223c<\/g:mo>\n                      <g:mn>2<\/g:mn>\n                      <g:mo>\u00d7<\/g:mo>\n                      <g:msup>\n                        <g:mn>10<\/g:mn>\n                        <g:mrow>\n                          <g:mo>\u2212<\/g:mo>\n                          <g:mn>13<\/g:mn>\n                        <\/g:mrow>\n                      <\/g:msup>\n                      <g:mtext>\u2009<\/g:mtext>\n                      <g:mtext>\u2009<\/g:mtext>\n                      <g:mi>eV<\/g:mi>\n                    <\/g:math>\n                    . For vectors with masses between\n                    <i:math xmlns:i=\"http:\/\/www.w3.org\/1998\/Math\/MathML\" display=\"inline\">\n                      <i:mrow>\n                        <i:mo stretchy=\"false\">[<\/i:mo>\n                        <i:mn>7<\/i:mn>\n                        <i:mo>\u00d7<\/i:mo>\n                        <i:msup>\n                          <i:mrow>\n                            <i:mn>10<\/i:mn>\n                          <\/i:mrow>\n                          <i:mrow>\n                            <i:mo>\u2212<\/i:mo>\n                            <i:mn>13<\/i:mn>\n                          <\/i:mrow>\n                        <\/i:msup>\n                        <i:mo>,<\/i:mo>\n                        <i:mn>8.47<\/i:mn>\n                        <i:mo>\u00d7<\/i:mo>\n                        <i:msup>\n                          <i:mrow>\n                            <i:mn>10<\/i:mn>\n                          <\/i:mrow>\n                          <i:mrow>\n                            <i:mo>\u2212<\/i:mo>\n                            <i:mn>12<\/i:mn>\n                          <\/i:mrow>\n                        <\/i:msup>\n                        <i:mo stretchy=\"false\">]<\/i:mo>\n                        <i:mtext>\u2009<\/i:mtext>\n                        <i:mtext>\u2009<\/i:mtext>\n                        <i:mi>eV<\/i:mi>\n                      <\/i:mrow>\n                    <\/i:math>\n                    that couple to baryons, our constraints on the dark-photon or baryon coupling supersede those from MICROSCOPE and E\u00f6t-Wash by 1 to 2 orders of magnitude, reaching a minimum of\n                    <m:math xmlns:m=\"http:\/\/www.w3.org\/1998\/Math\/MathML\" display=\"inline\">\n                      <m:mo>\u223c<\/m:mo>\n                      <m:mn>5<\/m:mn>\n                      <m:mo>\u00d7<\/m:mo>\n                      <m:msup>\n                        <m:mn>10<\/m:mn>\n                        <m:mrow>\n                          <m:mo>\u2212<\/m:mo>\n                          <m:mn>24<\/m:mn>\n                        <\/m:mrow>\n                      <\/m:msup>\n                    <\/m:math>\n                    at a mass of\n                    <o:math xmlns:o=\"http:\/\/www.w3.org\/1998\/Math\/MathML\" display=\"inline\">\n                      <o:mo>\u223c<\/o:mo>\n                      <o:msup>\n                        <o:mn>10<\/o:mn>\n                        <o:mrow>\n                          <o:mo>\u2212<\/o:mo>\n                          <o:mn>12<\/o:mn>\n                        <\/o:mrow>\n                      <\/o:msup>\n                      <o:mtext>\u2009<\/o:mtext>\n                      <o:mtext>\u2009<\/o:mtext>\n                      <o:mi>eV<\/o:mi>\n                    <\/o:math>\n                    . For tensors with masses of\n                    <q:math xmlns:q=\"http:\/\/www.w3.org\/1998\/Math\/MathML\" display=\"inline\">\n                      <q:mrow>\n                        <q:mo stretchy=\"false\">[<\/q:mo>\n                        <q:mn>4<\/q:mn>\n                        <q:mo>\u00d7<\/q:mo>\n                        <q:msup>\n                          <q:mrow>\n                            <q:mn>10<\/q:mn>\n                          <\/q:mrow>\n                          <q:mrow>\n                            <q:mo>\u2212<\/q:mo>\n                            <q:mn>14<\/q:mn>\n                          <\/q:mrow>\n                        <\/q:msup>\n                        <q:mo>,<\/q:mo>\n                        <q:mn>8.47<\/q:mn>\n                        <q:mo>\u00d7<\/q:mo>\n                        <q:msup>\n                          <q:mrow>\n                            <q:mn>10<\/q:mn>\n                          <\/q:mrow>\n                          <q:mrow>\n                            <q:mo>\u2212<\/q:mo>\n                            <q:mn>12<\/q:mn>\n                          <\/q:mrow>\n                        <\/q:msup>\n                        <q:mo stretchy=\"false\">]<\/q:mo>\n                        <q:mtext>\u2009<\/q:mtext>\n                        <q:mtext>\u2009<\/q:mtext>\n                        <q:mi>eV<\/q:mi>\n                      <\/q:mrow>\n                    <\/q:math>\n                    (the full mass range analyzed) that couple via a Yukawa interaction, our constraints, which are the first obtained from gravitational-wave interferometers, surpass those from fifth-force experiments by 4 to 5 orders of magnitude, achieving a limit as low as\n                    <u:math xmlns:u=\"http:\/\/www.w3.org\/1998\/Math\/MathML\" display=\"inline\">\n                      <u:mo>\u223c<\/u:mo>\n                      <u:mn>8<\/u:mn>\n                      <u:mo>\u00d7<\/u:mo>\n                      <u:msup>\n                        <u:mn>10<\/u:mn>\n                        <u:mrow>\n                          <u:mo>\u2212<\/u:mo>\n                          <u:mn>9<\/u:mn>\n                        <\/u:mrow>\n                      <\/u:msup>\n                    <\/u:math>\n                    at\n                    <w:math xmlns:w=\"http:\/\/www.w3.org\/1998\/Math\/MathML\" display=\"inline\">\n                      <w:mo>\u223c<\/w:mo>\n                      <w:mn>2<\/w:mn>\n                      <w:mo>\u00d7<\/w:mo>\n                      <w:msup>\n                        <w:mn>10<\/w:mn>\n                        <w:mrow>\n                          <w:mo>\u2212<\/w:mo>\n                          <w:mn>13<\/w:mn>\n                        <\/w:mrow>\n                      <\/w:msup>\n                      <w:mtext>\u2009<\/w:mtext>\n                      <w:mtext>\u2009<\/w:mtext>\n                      <w:mi>eV<\/w:mi>\n                    <\/w:math>\n                    . Our results show that each method has substantially different sensitivity to each dark matter candidate, highlighting the importance of a multimethod approach to search for new physics. Moreover, they demonstrate that gravitational-wave interferometers can simultaneously probe multiple ultralight dark matter models and place unprecedented constraints on tensor fields arising in a broad range of modified-gravity theories.\n                  <\/jats:p>","DOI":"10.1103\/qdnd-rsnh","type":"journal-article","created":{"date-parts":[[2026,8,17]],"date-time":"2026-08-17T12:16:50Z","timestamp":1786969010000},"update-policy":"https:\/\/doi.org\/10.1103\/crossmark-policy","source":"Crossref","is-referenced-by-count":2,"title":["Direct Multimodel Dark Matter Search with Gravitational-Wave Interferometers Using Data from the First Part of the Fourth LIGO-Virgo-KAGRA Observing Run"],"prefix":"10.1103","volume":"137","author":[{"ORCID":"https:\/\/orcid.org\/0000-0003-4786-2698","authenticated-orcid":true,"given":"A.\u2009G.","family":"Abac","sequence":"first","affiliation":[{"name":"Max Planck Institute for Gravitational Physics (Albert Einstein 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